The complete scattering diagram \(\mathcal {D}_Q\)  is then determined from this initial data by consistency using the flow tree formula of [1]}, [2]}. By scaling invariance, the scattering diagram can be
restricted to the hyperplane \(\theta _1+\theta _2+\theta _3=1\) 
with no loss of information, except for the rays \(\mathcal {R}_o(\delta )\)  associated to D0-branes
which are no longer visible. The resulting
two-dimensional scattering diagram is shown in Figure REF ,
including only the initial rays and a few secondary rays.
<FIGURE>